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#1203
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What is the remainder when 152016 is divided by 11, please?

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And it needs to be solved without using any computing devices.
Всё не так плохо как Вы думаете. Всё намного хуже!
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#1204
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4. If a number x = a * 11 + b (where b is the remainder of the division), then x^2016 = A * 11 + b^2016, where A is some integer expression, a polynomial where the argument is the number 11. In fact, if x = 15, then b = 4. x^2016 = A * 11 + 2^4032 We notice: if the remainder were equal to 1, then 1 to any power would remain 1. For powers of two: 2^10 is divisible by 11 with a remainder of 1. Then 2^4032 = (2^10)^403 * 2^2 = (c * 11 + 1)^403 * 2^2 = (C * 11 + 1) * 2^2 It is clear that the final remainder is four.
 

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#1205
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Yes, 4. Guess, Ment.
Всё не так плохо как Вы думаете. Всё намного хуже!
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#1206
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Well, since nothing planned for the vacation actually worked out, with Ment's permission, I’ll at least pose a riddle. I myself solved it a very, very long time ago… Now I don’t even remember either the answer or how I solved it, but back then that guy said that I had solved it correctly, although his solution was much shorter and easier than mine. So here is the riddle, and I will try to find, recall, or re-solve it again. I’m not sure if I can solve it again, but here is the riddle. A hollow hemisphere of mass m lies on a table. Water begins to be poured into it from above through a small hole. To what height H will it fill up?
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Всё не так плохо как Вы думаете. Всё намного хуже!
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#1207
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Hermit, is the radius of the hemisphere known? If so, here it is: mg = integrate (h from 0 to H) ρgh*dS(h) = integrate (α from 0 to arcsin(H/R)) ρgRsin(α)*2π(Rcos(α))*dα = integrate (α from 0 to arcsin(H/R)) ρgR*π*sin(2α)*dα = -0.5πρgRcos(2α) (α from 0 to arcsin(H/R)) = -0.5πρgR (cos(2arcsin(H/R))-1) = -0.5πρgR (1-2(H/R)^2-1) = πρgR(H/R)^2 = πρgH^2/R H = sqrt(mR/πρg)
 

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#1208
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If it's needed, then prove it. I didn't delve into the solution because the dimension of the expression under the root is (kg*m)/((kg/m3)*(m/s2)) = (kg*m)*(m2*s2)/kg = m3*s2. After taking the square root, it will be m3/2*s, and height is measured only in meters to the first power and without any seconds...

Added 1 minute ago
Now I'll also try to understand the solution.

Added 10 minutes ago
From the very beginning, the pressure at height h will not be ρgh, because at the very bottom it will be the largest, and not zero...

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And, if possible, Ment, please provide more details, because the idea of the solution is absolutely correct, but the answer is not yet.
Всё не так плохо как Вы думаете. Всё намного хуже!
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#1209
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After extracting the square root, it will be m3/2*c, and the height is measured only in meters to the first power, without any seconds...
Yes, all the comments are correct. Tomorrow I will rewrite these integrals more carefully, because right now I've written some nonsense again...
 

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#1211
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We're here to degrade, we don't need your integrals.
А, вот почему.

🏹🎪+⛓️♿=💕
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#1212
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Down with mental activity!
aka Sir Holmes aka David Jones.
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#1213
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The first mistake was about the pressure being lower at the bottom. Let's correct it: mg = integrate (h from 0 to H) ρg(H-h)*dS(h) = integrate (h from 0 to H) ρgH*dS(h) - integrate (h from 0 to H) ρgh*dS(h) ------------- (1) The second mistake was forgetting R in one place when expanding the small area element dS, and then losing another R somewhere: integrate (h from 0 to H) ρgh*dS(h) = integrate (α from 0 to arcsin(H/R)) ρgRsin(α)*2π(Rcos(α))*Rdα = integrate (α from 0 to arcsin(H/R)) ρgR*π*sin(2α)*R^2*dα = -0.5πρgR^3cos(2α) (α from 0 to arcsin(H/R)) = -0.5πρgR^3 ( cos(2arcsin(H/R))-1) = -0.5πρgR^3 ( 1-2(H/R)^2-1) = πρgRH^2 -------------- (2) The first integral from the sum in (1): integrate (h from 0 to H) ρgH*dS(h) = integrate (α from 0 to arcsin(H/R)) ρgH*2π(Rcos(α))R*dα = 2πρgHR^2 * integrate (α from 0 to arcsin(H/R)) cos(α)dα = 2πρgHR^2 * sin(α) (α from 0 to arcsin(H/R)) = 2πρgHR^2 * H/R = 2πρgRH^2 (3) Let's combine (1), (2), and (3), and remember to cancel out g from both parts, which I forgot to do last time. m = 2πρRH^2 - πρRH^2 = πρRH^2 H = sqrt(m/πρR) If needed, I won't ask for another attempt, as there's nothing more to do for now.
 

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#1214
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The dimensions are correct here; I'll take a look at the solution now. I solved it again, but my answer seems to be incorrect...
Всё не так плохо как Вы думаете. Всё намного хуже!
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#1216
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Why are you simply arithmetically adding the forces ρg(H-h)*dS(h) with which the water presses on infinitely small strips?

Added after 39 seconds
Ment
Does R enter into it?
I won't say. ;)
Всё не так плохо как Вы думаете. Всё намного хуже!
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#1217
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HoM[M]ie
Down with mental activity!
Drakkoska
We came here to degrade; we don't need your integrals.
There you can degrade; leave this place for us...:mad::mad::mad:

Ничто не возникает из ничего и ничто не пропадает бесследно.
Если где-то чего-то убудет, то в другом месте добавится.

(Закон сохранения).